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Groups > sci.physics.relativity > #614841 > unrolled thread
| Started by | Laurence Clark Crossen <l.c.crossen@hotmail.com> |
|---|---|
| First post | 2023-07-09 10:56 -0700 |
| Last post | 2023-07-11 13:02 -0700 |
| Articles | 19 on this page of 39 — 14 participants |
Back to article view | Back to sci.physics.relativity
A light clock that works. Laurence Clark Crossen <l.c.crossen@hotmail.com> - 2023-07-09 10:56 -0700
Re: A light clock that works. "mitchr...@gmail.com" <mitchrae3323@gmail.com> - 2023-07-09 11:11 -0700
Re: A light clock that works. Laurence Clark Crossen <l.c.crossen@hotmail.com> - 2023-07-09 12:02 -0700
Re: A light clock that works. Bill <davos2329@gmail.com> - 2023-07-09 11:21 -0700
Re: A light clock that works. Laurence Clark Crossen <l.c.crossen@hotmail.com> - 2023-07-09 12:04 -0700
Re: A light clock that works. Bill <davos2329@gmail.com> - 2023-07-09 12:29 -0700
Re: A light clock that works. Laurence Clark Crossen <l.c.crossen@hotmail.com> - 2023-07-09 12:39 -0700
Re: A light clock that works. Bill <davos2329@gmail.com> - 2023-07-09 13:53 -0700
Re: A light clock that works. whodat <whodaat@void.nowgre.com> - 2023-07-09 16:13 -0500
Re: A light clock that works. nospam@de-ster.demon.nl (J. J. Lodder) - 2023-07-09 22:54 +0200
Re: A light clock that works. Laurence Clark Crossen <l.c.crossen@hotmail.com> - 2023-07-09 15:06 -0700
Re: A light clock that works. Bill <davos2329@gmail.com> - 2023-07-09 16:25 -0700
Re: A light clock that works. whodat <whodaat@void.nowgre.com> - 2023-07-09 21:08 -0500
Re: A light clock that works. Laurence Clark Crossen <l.c.crossen@hotmail.com> - 2023-07-10 09:32 -0700
Re: A light clock that works. Bill <davos2329@gmail.com> - 2023-07-10 11:49 -0700
Re: A light clock that works. Bill <davos2329@gmail.com> - 2023-07-10 11:53 -0700
Re: A light clock that works. whodat <whodaat@void.nowgre.com> - 2023-07-10 14:16 -0500
Re: A light clock that works. Mikko <mikko.levanto@iki.fi> - 2023-07-10 11:13 +0300
Re: A light clock that works. Maciej Wozniak <maluwozniak@gmail.com> - 2023-07-10 01:42 -0700
Re: A light clock that works. Sylvia Else <sylvia@email.invalid> - 2023-07-10 22:11 +1000
Re: A light clock that works. Laurence Clark Crossen <l.c.crossen@hotmail.com> - 2023-07-10 06:12 -0700
Re: A light clock that works. Sylvia Else <sylvia@email.invalid> - 2023-07-10 23:22 +1000
Re: A light clock that works. Laurence Clark Crossen <l.c.crossen@hotmail.com> - 2023-07-10 06:58 -0700
Re: A light clock that works. Sylvia Else <sylvia@email.invalid> - 2023-07-11 00:09 +1000
Re: A light clock that works. Laurence Clark Crossen <l.c.crossen@hotmail.com> - 2023-07-10 07:11 -0700
Re: A light clock that works. Laurence Clark Crossen <l.c.crossen@hotmail.com> - 2023-07-10 07:22 -0700
Re: A light clock that works. Richard Hachel <r.hachel@frite.fr> - 2023-07-10 14:32 +0000
Re: A light clock that works. Athel Cornish-Bowden <athel.cb@gmail.com> - 2023-07-10 16:56 +0200
Re: A light clock that works. Jhon-Jhairo Papadopulos <drao@ohuholsj.jo> - 2023-07-10 17:28 +0000
Re: A light clock that works. Pablo Sfakianos <lsop@saikfiof.sn> - 2023-07-10 19:45 +0000
Re: A light clock that works. Laurence Clark Crossen <l.c.crossen@hotmail.com> - 2023-07-10 08:19 -0700
Re: A light clock that works. Sylvia Else <sylvia@email.invalid> - 2023-07-11 11:23 +1000
Re: A light clock that works. whodat <whodaat@void.nowgre.com> - 2023-07-10 20:54 -0500
Re: A light clock that works. Laurence Clark Crossen <l.c.crossen@hotmail.com> - 2023-07-10 07:10 -0700
Re: A light clock that works. wugi <wugi@brol.invalid> - 2023-07-10 21:52 +0200
Re: A light clock that works. Laurence Clark Crossen <l.c.crossen@hotmail.com> - 2023-07-11 10:56 -0700
Re: A light clock that works. Richard Hachel <r.hachel@frite.fr> - 2023-07-11 18:17 +0000
Re: A light clock that works. Tom Roberts <tjoberts137@sbcglobal.net> - 2023-07-11 13:22 -0500
Re: A light clock that works. Maciej Wozniak <maluwozniak@gmail.com> - 2023-07-11 13:02 -0700
Page 2 of 2 — ← Prev page 1 [2]
| From | Laurence Clark Crossen <l.c.crossen@hotmail.com> |
|---|---|
| Date | 2023-07-10 06:12 -0700 |
| Message-ID | <e4d1263c-19d5-43be-a0c1-fb4220a38d05n@googlegroups.com> |
| In reply to | #614903 |
On Monday, July 10, 2023 at 5:11:45 AM UTC-7, Sylvia Else wrote: > On 10-July-23 3:56 am, Laurence Clark Crossen wrote: > > Design of a light clock that works on a spaceship traveling at near the speed of light: > > Orient a light clock horizontally like the beam in the MMX directed in the direction of Earth's orbital motion. > > The beam going out to the mirror is in the direction of the spaceship's motion. > > That beam covers a longer distance since that mirror is moving away > > On the return trip, it covers a shorter distance because the other side of the clock is moving towards it. > > Result: The clock functions at the same rate as when stationary. > > Further: This works whether light shares the velocity of the source or not. > > Question: Why did Einstein choose a clock that doesn't work when an available one does? > Care to expand on that using algebra, rather than hand-waving? > > Sylvia. I would have thought you knew elementary algebra. With light speed independent of the speed of the source: Distance= (d + x) + (d - x)= 2d. Velocity= c Time= 2d/c In case you didn't understand, refer to the completely sufficient verbal description given previously.
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| From | Sylvia Else <sylvia@email.invalid> |
|---|---|
| Date | 2023-07-10 23:22 +1000 |
| Message-ID | <kh2evqF3oq5U1@mid.individual.net> |
| In reply to | #614904 |
On 10-July-23 11:12 pm, Laurence Clark Crossen wrote: > On Monday, July 10, 2023 at 5:11:45 AM UTC-7, Sylvia Else wrote: >> On 10-July-23 3:56 am, Laurence Clark Crossen wrote: >>> Design of a light clock that works on a spaceship traveling at near the speed of light: >>> Orient a light clock horizontally like the beam in the MMX directed in the direction of Earth's orbital motion. >>> The beam going out to the mirror is in the direction of the spaceship's motion. >>> That beam covers a longer distance since that mirror is moving away >>> On the return trip, it covers a shorter distance because the other side of the clock is moving towards it. >>> Result: The clock functions at the same rate as when stationary. >>> Further: This works whether light shares the velocity of the source or not. >>> Question: Why did Einstein choose a clock that doesn't work when an available one does? >> Care to expand on that using algebra, rather than hand-waving? >> >> Sylvia. > I would have thought you knew elementary algebra. > With light speed independent of the speed of the source: > Distance= (d + x) + (d - x)= 2d. > Velocity= c > Time= 2d/c > In case you didn't understand, refer to the completely sufficient verbal description given previously. You said near the speed of light, presumably relative to some as yet to be identified observer, since it cannot be relative to the spaceship itself. Sylvia.
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| From | Laurence Clark Crossen <l.c.crossen@hotmail.com> |
|---|---|
| Date | 2023-07-10 06:58 -0700 |
| Message-ID | <1ef8da5b-ef9d-4487-807b-175ca855d312n@googlegroups.com> |
| In reply to | #614905 |
On Monday, July 10, 2023 at 6:22:07 AM UTC-7, Sylvia Else wrote: > On 10-July-23 11:12 pm, Laurence Clark Crossen wrote: > > On Monday, July 10, 2023 at 5:11:45 AM UTC-7, Sylvia Else wrote: > >> On 10-July-23 3:56 am, Laurence Clark Crossen wrote: > >>> Design of a light clock that works on a spaceship traveling at near the speed of light: > >>> Orient a light clock horizontally like the beam in the MMX directed in the direction of Earth's orbital motion. > >>> The beam going out to the mirror is in the direction of the spaceship's motion. > >>> That beam covers a longer distance since that mirror is moving away > >>> On the return trip, it covers a shorter distance because the other side of the clock is moving towards it. > >>> Result: The clock functions at the same rate as when stationary. > >>> Further: This works whether light shares the velocity of the source or not. > >>> Question: Why did Einstein choose a clock that doesn't work when an available one does? > >> Care to expand on that using algebra, rather than hand-waving? > >> > >> Sylvia. > > I would have thought you knew elementary algebra. > > With light speed independent of the speed of the source: > > Distance= (d + x) + (d - x)= 2d. > > Velocity= c > > Time= 2d/c > > In case you didn't understand, refer to the completely sufficient verbal description given previously. > You said near the speed of light, presumably relative to some as yet to > be identified observer, since it cannot be relative to the spaceship itself. > > Sylvia. How needlessly you complicate matters. The observer reading the light clock is inside the ship.
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| From | Sylvia Else <sylvia@email.invalid> |
|---|---|
| Date | 2023-07-11 00:09 +1000 |
| Message-ID | <kh2hoeF3oq2U1@mid.individual.net> |
| In reply to | #614906 |
On 10-July-23 11:58 pm, Laurence Clark Crossen wrote: > On Monday, July 10, 2023 at 6:22:07 AM UTC-7, Sylvia Else wrote: >> On 10-July-23 11:12 pm, Laurence Clark Crossen wrote: >>> On Monday, July 10, 2023 at 5:11:45 AM UTC-7, Sylvia Else wrote: >>>> On 10-July-23 3:56 am, Laurence Clark Crossen wrote: >>>>> Design of a light clock that works on a spaceship traveling at near the speed of light: >>>>> Orient a light clock horizontally like the beam in the MMX directed in the direction of Earth's orbital motion. >>>>> The beam going out to the mirror is in the direction of the spaceship's motion. >>>>> That beam covers a longer distance since that mirror is moving away >>>>> On the return trip, it covers a shorter distance because the other side of the clock is moving towards it. >>>>> Result: The clock functions at the same rate as when stationary. >>>>> Further: This works whether light shares the velocity of the source or not. >>>>> Question: Why did Einstein choose a clock that doesn't work when an available one does? >>>> Care to expand on that using algebra, rather than hand-waving? >>>> >>>> Sylvia. >>> I would have thought you knew elementary algebra. >>> With light speed independent of the speed of the source: >>> Distance= (d + x) + (d - x)= 2d. >>> Velocity= c >>> Time= 2d/c >>> In case you didn't understand, refer to the completely sufficient verbal description given previously. >> You said near the speed of light, presumably relative to some as yet to >> be identified observer, since it cannot be relative to the spaceship itself. >> >> Sylvia. > How needlessly you complicate matters. The observer reading the light clock is inside the ship. So what do you mean by "travelling at near the speed of light"? How would someone determine that they were, or were not, travelling at near the speed of light? Sylvia.
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| From | Laurence Clark Crossen <l.c.crossen@hotmail.com> |
|---|---|
| Date | 2023-07-10 07:11 -0700 |
| Message-ID | <b09432b2-22fa-459a-8065-ff7fac91c429n@googlegroups.com> |
| In reply to | #614907 |
On Monday, July 10, 2023 at 7:09:23 AM UTC-7, Sylvia Else wrote: > On 10-July-23 11:58 pm, Laurence Clark Crossen wrote: > > On Monday, July 10, 2023 at 6:22:07 AM UTC-7, Sylvia Else wrote: > >> On 10-July-23 11:12 pm, Laurence Clark Crossen wrote: > >>> On Monday, July 10, 2023 at 5:11:45 AM UTC-7, Sylvia Else wrote: > >>>> On 10-July-23 3:56 am, Laurence Clark Crossen wrote: > >>>>> Design of a light clock that works on a spaceship traveling at near the speed of light: > >>>>> Orient a light clock horizontally like the beam in the MMX directed in the direction of Earth's orbital motion. > >>>>> The beam going out to the mirror is in the direction of the spaceship's motion. > >>>>> That beam covers a longer distance since that mirror is moving away > >>>>> On the return trip, it covers a shorter distance because the other side of the clock is moving towards it. > >>>>> Result: The clock functions at the same rate as when stationary. > >>>>> Further: This works whether light shares the velocity of the source or not. > >>>>> Question: Why did Einstein choose a clock that doesn't work when an available one does? > >>>> Care to expand on that using algebra, rather than hand-waving? > >>>> > >>>> Sylvia. > >>> I would have thought you knew elementary algebra. > >>> With light speed independent of the speed of the source: > >>> Distance= (d + x) + (d - x)= 2d. > >>> Velocity= c > >>> Time= 2d/c > >>> In case you didn't understand, refer to the completely sufficient verbal description given previously. > >> You said near the speed of light, presumably relative to some as yet to > >> be identified observer, since it cannot be relative to the spaceship itself. > >> > >> Sylvia. > > How needlessly you complicate matters. The observer reading the light clock is inside the ship. > So what do you mean by "travelling at near the speed of light"? How > would someone determine that they were, or were not, travelling at near > the speed of light? > > Sylvia. Nobody is hoodwinked by relativity here. The spaceship has a speedometer.
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| From | Laurence Clark Crossen <l.c.crossen@hotmail.com> |
|---|---|
| Date | 2023-07-10 07:22 -0700 |
| Message-ID | <baaaf7f9-f4cc-4583-b8a8-3e1520079538n@googlegroups.com> |
| In reply to | #614907 |
On Monday, July 10, 2023 at 7:09:23 AM UTC-7, Sylvia Else wrote: > On 10-July-23 11:58 pm, Laurence Clark Crossen wrote: > > On Monday, July 10, 2023 at 6:22:07 AM UTC-7, Sylvia Else wrote: > >> On 10-July-23 11:12 pm, Laurence Clark Crossen wrote: > >>> On Monday, July 10, 2023 at 5:11:45 AM UTC-7, Sylvia Else wrote: > >>>> On 10-July-23 3:56 am, Laurence Clark Crossen wrote: > >>>>> Design of a light clock that works on a spaceship traveling at near the speed of light: > >>>>> Orient a light clock horizontally like the beam in the MMX directed in the direction of Earth's orbital motion. > >>>>> The beam going out to the mirror is in the direction of the spaceship's motion. > >>>>> That beam covers a longer distance since that mirror is moving away > >>>>> On the return trip, it covers a shorter distance because the other side of the clock is moving towards it. > >>>>> Result: The clock functions at the same rate as when stationary. > >>>>> Further: This works whether light shares the velocity of the source or not. > >>>>> Question: Why did Einstein choose a clock that doesn't work when an available one does? > >>>> Care to expand on that using algebra, rather than hand-waving? > >>>> > >>>> Sylvia. > >>> I would have thought you knew elementary algebra. > >>> With light speed independent of the speed of the source: > >>> Distance= (d + x) + (d - x)= 2d. > >>> Velocity= c > >>> Time= 2d/c > >>> In case you didn't understand, refer to the completely sufficient verbal description given previously. > >> You said near the speed of light, presumably relative to some as yet to > >> be identified observer, since it cannot be relative to the spaceship itself. > >> > >> Sylvia. > > How needlessly you complicate matters. The observer reading the light clock is inside the ship. > So what do you mean by "travelling at near the speed of light"? How > would someone determine that they were, or were not, travelling at near > the speed of light? > > Sylvia. In Galileo's ship you can look out the window and know it's moving.
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| From | Richard Hachel <r.hachel@frite.fr> |
|---|---|
| Date | 2023-07-10 14:32 +0000 |
| Message-ID | <IbkTVEhLGrybRFhrnx3L1hwga6M@jntp> |
| In reply to | #614910 |
Le 10/07/2023 à 16:22, Laurence Clark Crossen a écrit : > On Monday, July 10, 2023 at 7:09:23 AM UTC-7, Sylvia Else wrote: >> On 10-July-23 11:58 pm, Laurence Clark Crossen wrote: >> > On Monday, July 10, 2023 at 6:22:07 AM UTC-7, Sylvia Else wrote: >> >> On 10-July-23 11:12 pm, Laurence Clark Crossen wrote: >> >>> On Monday, July 10, 2023 at 5:11:45 AM UTC-7, Sylvia Else wrote: >> >>>> On 10-July-23 3:56 am, Laurence Clark Crossen wrote: >> >>>>> Design of a light clock that works on a spaceship traveling at near the >> speed of light: >> >>>>> Orient a light clock horizontally like the beam in the MMX directed in the >> direction of Earth's orbital motion. >> >>>>> The beam going out to the mirror is in the direction of the spaceship's >> motion. >> >>>>> That beam covers a longer distance since that mirror is moving away >> >>>>> On the return trip, it covers a shorter distance because the other side of >> the clock is moving towards it. >> >>>>> Result: The clock functions at the same rate as when stationary. >> >>>>> Further: This works whether light shares the velocity of the source or >> not. >> >>>>> Question: Why did Einstein choose a clock that doesn't work when an >> available one does? >> >>>> Care to expand on that using algebra, rather than hand-waving? >> >>>> >> >>>> Sylvia. >> >>> I would have thought you knew elementary algebra. >> >>> With light speed independent of the speed of the source: >> >>> Distance= (d + x) + (d - x)= 2d. >> >>> Velocity= c >> >>> Time= 2d/c >> >>> In case you didn't understand, refer to the completely sufficient verbal >> description given previously. >> >> You said near the speed of light, presumably relative to some as yet to >> >> be identified observer, since it cannot be relative to the spaceship itself. >> >> >> >> Sylvia. >> > How needlessly you complicate matters. The observer reading the light clock is >> inside the ship. >> So what do you mean by "travelling at near the speed of light"? How >> would someone determine that they were, or were not, travelling at near >> the speed of light? >> >> Sylvia. > In Galileo's ship you can look out the window and know it's moving. Certainly, but in Dr. Hachel's ship, there is no absolute frame of reference (like a fixed and immutable ether). If we admit that the universe does not exist, and that there are no stars, no planets, but only a rocket that wanders in the empty and infinite spaces. It is clear that she would not move, nor could she be moved. Not everything is "sex". Look at Snow White and the Seven Dwarfs. Wonderful Walt Disney movie. But where are the space and the time during which we shot the film? Where is the house that served as a spatial support? But no, it's just colors on film. There is nothing absolute here. Same in our universe. Everything is only by comparisons of colors of distances, of time. But no absolute reference. Let's take the notion of speed: which of A or B is really going faster? A is at rest, and says that it is B who moves and therefore goes faster. B looks at A wryly and says: "No, you're the one going faster!". R.H.
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| From | Athel Cornish-Bowden <athel.cb@gmail.com> |
|---|---|
| Date | 2023-07-10 16:56 +0200 |
| Message-ID | <kh2kh0F4lfoU1@mid.individual.net> |
| In reply to | #614911 |
On 2023-07-10 14:32:27 +0000, "Dr." Richard Hachel said: >>> >>> [ … ] >>> > Certainly, but in Dr. Hachel's ship, there is no absolute frame of > reference (like a fixed and immutable ether). All very interesting, but you still haven't revealed where you earned your doctorate. > > If we admit that the universe does not exist, and that there are no > stars, no planets, but only a rocket that wanders in the empty and > infinite spaces. > > It is clear that she would not move, nor could she be moved. > > Not everything is "sex". > > Look at Snow White and the Seven Dwarfs. > > Wonderful Walt Disney movie. > > But where are the space and the time during which we shot the film? > Where is the house that served as a spatial support? > > But no, it's just colors on film. > > There is nothing absolute here. > > Same in our universe. Everything is only by comparisons of colors of > distances, of time. > > But no absolute reference. > > Let's take the notion of speed: which of A or B is really going faster? > > A is at rest, and says that it is B who moves and therefore goes faster. > > B looks at A wryly and says: "No, you're the one going faster!". > > R.H. -- athel -- biochemist, not a physicist, but detector of crackpots
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| From | Jhon-Jhairo Papadopulos <drao@ohuholsj.jo> |
|---|---|
| Date | 2023-07-10 17:28 +0000 |
| Message-ID | <u8hf41$ljtd$1@paganini.bofh.team> |
| In reply to | #614912 |
Athel Cornish-Bowden wrote: > On 2023-07-10 14:32:27 +0000, "Dr." Richard Hachel said: >> Certainly, but in Dr. Hachel's ship, there is no absolute frame of >> reference (like a fixed and immutable ether). > > All very interesting, but you still haven't revealed where you earned > your doctorate. everybody really undrestand this title here, really undrestand?? With your money, he stole from you, he is walking alive and depopulate. You stinking capitalists, what the fuck is wrong with you. *_WHO_To_Flood_Africa_With_Bill_Gates’_Experimental_Malaria_Vaccine_* To ‘Fight Climate Change’ https://thepeoplesvoice.tv/who-to-flood-africa-with-bill-gates-experimental-malaria-vaccine-to-fight-climate-change/ *_WEF_Says_CBDCs_Must_Be_‘Implanted_Under_Your_Skin’_* if You Want To Participate in Society https://thepeoplesvoice.tv/wef-says-cbdcs-must-be-implanted-under-your-skin-if-you-want-to-participate-in-society/ *_Biological_Man_Wins_This_Years_“Miss_Netherlands”_* https://thepeoplesvoice.tv/biological-man-wins-this-years-miss-netherlands/
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| From | Pablo Sfakianos <lsop@saikfiof.sn> |
|---|---|
| Date | 2023-07-10 19:45 +0000 |
| Message-ID | <u8hn53$ljtd$2@paganini.bofh.team> |
| In reply to | #614918 |
mitchr...@gmail.com wrote: >> *_WHO_To_Flood_Africa_With_Bill_Gates’_Experimental_Malaria_Vaccine_* To >> ‘Fight Climate Change’ >> >> https://thepeoplesvoice.tv/who-to-flood-africa-with-bill-gates-experimental-malaria-vaccine-to-fight-climate-change/ >> >> *_WEF_Says_CBDCs_Must_Be_‘Implanted_Under_Your_Skin’_* if You Want To >> Participate in Society >> https://thepeoplesvoice.tv/wef-says-cbdcs-must-be-implanted-under-your-skin-if-you-want-to-participate-in-society/ >> >> *_Biological_Man_Wins_This_Years_“Miss_Netherlands”_* >> https://thepeoplesvoice.tv/biological-man-wins-this-years-miss-netherlands/ > > If light is propagating how do we see it in free space? > Does it not have to absorb? sure it does. It has to scatter or reflect from some piece of matter, otherwise it's invisible in all countries, and you can't see it. nor care. Fully based on my *_"On_the_Divergent_Mater_of_the_Moving_Koepers_Model"_*.
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| From | Laurence Clark Crossen <l.c.crossen@hotmail.com> |
|---|---|
| Date | 2023-07-10 08:19 -0700 |
| Message-ID | <9e108ea9-8d6b-4b22-8dbc-5d16a4ffad7bn@googlegroups.com> |
| In reply to | #614907 |
On Monday, July 10, 2023 at 7:09:23 AM UTC-7, Sylvia Else wrote: > On 10-July-23 11:58 pm, Laurence Clark Crossen wrote: > > On Monday, July 10, 2023 at 6:22:07 AM UTC-7, Sylvia Else wrote: > >> On 10-July-23 11:12 pm, Laurence Clark Crossen wrote: > >>> On Monday, July 10, 2023 at 5:11:45 AM UTC-7, Sylvia Else wrote: > >>>> On 10-July-23 3:56 am, Laurence Clark Crossen wrote: > >>>>> Design of a light clock that works on a spaceship traveling at near the speed of light: > >>>>> Orient a light clock horizontally like the beam in the MMX directed in the direction of Earth's orbital motion. > >>>>> The beam going out to the mirror is in the direction of the spaceship's motion. > >>>>> That beam covers a longer distance since that mirror is moving away > >>>>> On the return trip, it covers a shorter distance because the other side of the clock is moving towards it. > >>>>> Result: The clock functions at the same rate as when stationary. > >>>>> Further: This works whether light shares the velocity of the source or not. > >>>>> Question: Why did Einstein choose a clock that doesn't work when an available one does? > >>>> Care to expand on that using algebra, rather than hand-waving? > >>>> > >>>> Sylvia. > >>> I would have thought you knew elementary algebra. > >>> With light speed independent of the speed of the source: > >>> Distance= (d + x) + (d - x)= 2d. > >>> Velocity= c > >>> Time= 2d/c > >>> In case you didn't understand, refer to the completely sufficient verbal description given previously. > >> You said near the speed of light, presumably relative to some as yet to > >> be identified observer, since it cannot be relative to the spaceship itself. > >> > >> Sylvia. > > How needlessly you complicate matters. The observer reading the light clock is inside the ship. > So what do you mean by "travelling at near the speed of light"? How > would someone determine that they were, or were not, travelling at near > the speed of light? > > Sylvia. There is only one geometry. The actual path of the light. Objective reality sans subjectivism.
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| From | Sylvia Else <sylvia@email.invalid> |
|---|---|
| Date | 2023-07-11 11:23 +1000 |
| Message-ID | <kh3p94Fabl0U1@mid.individual.net> |
| In reply to | #614913 |
On 11-July-23 1:19 am, Laurence Clark Crossen wrote: > On Monday, July 10, 2023 at 7:09:23 AM UTC-7, Sylvia Else wrote: >> On 10-July-23 11:58 pm, Laurence Clark Crossen wrote: >>> On Monday, July 10, 2023 at 6:22:07 AM UTC-7, Sylvia Else wrote: >>>> On 10-July-23 11:12 pm, Laurence Clark Crossen wrote: >>>>> On Monday, July 10, 2023 at 5:11:45 AM UTC-7, Sylvia Else wrote: >>>>>> On 10-July-23 3:56 am, Laurence Clark Crossen wrote: >>>>>>> Design of a light clock that works on a spaceship traveling at near the speed of light: >>>>>>> Orient a light clock horizontally like the beam in the MMX directed in the direction of Earth's orbital motion. >>>>>>> The beam going out to the mirror is in the direction of the spaceship's motion. >>>>>>> That beam covers a longer distance since that mirror is moving away >>>>>>> On the return trip, it covers a shorter distance because the other side of the clock is moving towards it. >>>>>>> Result: The clock functions at the same rate as when stationary. >>>>>>> Further: This works whether light shares the velocity of the source or not. >>>>>>> Question: Why did Einstein choose a clock that doesn't work when an available one does? >>>>>> Care to expand on that using algebra, rather than hand-waving? >>>>>> >>>>>> Sylvia. >>>>> I would have thought you knew elementary algebra. >>>>> With light speed independent of the speed of the source: >>>>> Distance= (d + x) + (d - x)= 2d. >>>>> Velocity= c >>>>> Time= 2d/c >>>>> In case you didn't understand, refer to the completely sufficient verbal description given previously. >>>> You said near the speed of light, presumably relative to some as yet to >>>> be identified observer, since it cannot be relative to the spaceship itself. >>>> >>>> Sylvia. >>> How needlessly you complicate matters. The observer reading the light clock is inside the ship. >> So what do you mean by "travelling at near the speed of light"? How >> would someone determine that they were, or were not, travelling at near >> the speed of light? >> >> Sylvia. > There is only one geometry. The actual path of the light. Objective reality sans subjectivism. You appear to unable to answer even simple questions about the terminology you used. Sylvia.
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| From | whodat <whodaat@void.nowgre.com> |
|---|---|
| Date | 2023-07-10 20:54 -0500 |
| Message-ID | <kh3r1rFaigoU2@mid.individual.net> |
| In reply to | #614960 |
On 7/10/2023 8:23 PM, Sylvia Else wrote: > On 11-July-23 1:19 am, Laurence Clark Crossen wrote: <...> >>>> How needlessly you complicate matters. The observer reading the >>>> light clock is inside the ship. >>> So what do you mean by "travelling at near the speed of light"? How >>> would someone determine that they were, or were not, travelling at near >>> the speed of light? >>> >>> Sylvia. >> There is only one geometry. The actual path of the light. Objective >> reality sans subjectivism. > > You appear to unable to answer even simple questions about the > terminology you used. Haven't you noticed the patterns?
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| From | Laurence Clark Crossen <l.c.crossen@hotmail.com> |
|---|---|
| Date | 2023-07-10 07:10 -0700 |
| Message-ID | <8ba1763c-d608-4167-bce6-514ad01b8f98n@googlegroups.com> |
| In reply to | #614905 |
On Monday, July 10, 2023 at 6:22:07 AM UTC-7, Sylvia Else wrote: > On 10-July-23 11:12 pm, Laurence Clark Crossen wrote: > > On Monday, July 10, 2023 at 5:11:45 AM UTC-7, Sylvia Else wrote: > >> On 10-July-23 3:56 am, Laurence Clark Crossen wrote: > >>> Design of a light clock that works on a spaceship traveling at near the speed of light: > >>> Orient a light clock horizontally like the beam in the MMX directed in the direction of Earth's orbital motion. > >>> The beam going out to the mirror is in the direction of the spaceship's motion. > >>> That beam covers a longer distance since that mirror is moving away > >>> On the return trip, it covers a shorter distance because the other side of the clock is moving towards it. > >>> Result: The clock functions at the same rate as when stationary. > >>> Further: This works whether light shares the velocity of the source or not. > >>> Question: Why did Einstein choose a clock that doesn't work when an available one does? > >> Care to expand on that using algebra, rather than hand-waving? > >> > >> Sylvia. > > I would have thought you knew elementary algebra. > > With light speed independent of the speed of the source: > > Distance= (d + x) + (d - x)= 2d. > > Velocity= c > > Time= 2d/c > > In case you didn't understand, refer to the completely sufficient verbal description given previously. > You said near the speed of light, presumably relative to some as yet to > be identified observer, since it cannot be relative to the spaceship itself. > > Sylvia. It doesn't matter where the observer is because the geometry is exactly the same. For example, in Galileo's ship cabin the ball bouncing up and down from ceiling to floor seems to cover only that distance but the observer can understand that because the ship is moving it is moving further.
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| From | wugi <wugi@brol.invalid> |
|---|---|
| Date | 2023-07-10 21:52 +0200 |
| Message-ID | <u8hnim$2k428$1@dont-email.me> |
| In reply to | #614841 |
Op 9/07/2023 om 19:56 schreef Laurence Clark Crossen: > Design of a light clock that works on a spaceship traveling at near the speed of light: > Orient a light clock horizontally like the beam in the MMX directed in the direction of Earth's orbital motion. > The beam going out to the mirror is in the direction of the spaceship's motion. > That beam covers a longer distance since that mirror is moving away > On the return trip, it covers a shorter distance because the other side of the clock is moving towards it. > Result: The clock functions at the same rate as when stationary. > Further: This works whether light shares the velocity of the source or not. > Question: Why did Einstein choose a clock that doesn't work when an available one does? Light clocks deserve indeed to be considered as *the* measuring and calibrating tools for both time and space in SRT. They allow even an axiomatic approach that is intuitive, and yields constant light speed as a provable result, rather than it being a counterintuitive axiom, as in the original formulation. But then it takes understanding their functioning. "Your" light clock works only for particle behaviour of light, with added velocities. Then you get indeed this: https://wugi.be/giffls/tik19.htm and tN = t'N'. But with wave/particle behaviour this is no longer true. Looking at such light clocks we see, first, that a "moving" light clock must suffer time dilation (longer light path perpendicular to direction of motion); then, that they must suffer length contraction (for parallel en perpendicular light paths to "ticktock" in pace: one wants *time* to be an isotropic feature); As a result we get this correct spacetime diagram for light clocks: https://wugi.be/giffls/tik22.htm. Furthermore, we see, that simultaneity is different in a "moving" system; and again, that these features are reciprocal: "moving" and "rest" systems can be swapped, with reciprocal results; lastly, that light speed is constant: light clocks measure by definition light speed as the ratio of corresponding ticktock lengths and time intervals! One can even deduce relativistic mass from light clock behaviour, by considering corresponding wavelengths and the light impulses involved. Hereafter you can toy with interactive graphs for the principal lightclock features: time dilation https://www.desmos.com/calculator/zlplep7g5k?lang=nl length contraction https://www.desmos.com/calculator/hpxundkvzt?lang=nl relative simultaneity https://www.desmos.com/calculator/7h1h4jvzno?lang=nl Also interesting, a difference between the mentioned "Lorentz" properties of relativistic motion, and the properties actually "seen when looking at" such motion. Other files about this theme, in my desmos space. -- guido wugi
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| From | Laurence Clark Crossen <l.c.crossen@hotmail.com> |
|---|---|
| Date | 2023-07-11 10:56 -0700 |
| Message-ID | <958e9961-71cf-410c-a405-d608390deadan@googlegroups.com> |
| In reply to | #614941 |
On Monday, July 10, 2023 at 12:52:57 PM UTC-7, wugi wrote: > Op 9/07/2023 om 19:56 schreef Laurence Clark Crossen: > > Design of a light clock that works on a spaceship traveling at near the speed of light: > > Orient a light clock horizontally like the beam in the MMX directed in the direction of Earth's orbital motion. > > The beam going out to the mirror is in the direction of the spaceship's motion. > > That beam covers a longer distance since that mirror is moving away > > On the return trip, it covers a shorter distance because the other side of the clock is moving towards it. > > Result: The clock functions at the same rate as when stationary. > > Further: This works whether light shares the velocity of the source or not. > > Question: Why did Einstein choose a clock that doesn't work when an available one does? > Light clocks deserve indeed to be considered as *the* measuring and > calibrating tools for both time and space in SRT. They allow even an > axiomatic approach that is intuitive, and yields constant light speed as > a provable result, rather than it being a counterintuitive axiom, as in > the original formulation. But then it takes understanding their functioning. > > "Your" light clock works only for particle behaviour of light, with > added velocities. Then you get indeed this: > https://wugi.be/giffls/tik19.htm > and tN = t'N'. > But with wave/particle behaviour this is no longer true. Looking at such > light clocks we see, > first, that a "moving" light clock must suffer time dilation (longer > light path perpendicular to direction of motion); > then, that they must suffer length contraction (for parallel en > perpendicular light paths to "ticktock" in pace: one wants *time* to be > an isotropic feature); > As a result we get this correct spacetime diagram for light clocks: > https://wugi.be/giffls/tik22.htm. > > Furthermore, we see, > that simultaneity is different in a "moving" system; > and again, that these features are reciprocal: "moving" and "rest" > systems can be swapped, with reciprocal results; > lastly, that light speed is constant: light clocks measure by definition > light speed as the ratio of corresponding ticktock lengths and time > intervals! > One can even deduce relativistic mass from light clock behaviour, by > considering corresponding wavelengths and the light impulses involved. > > Hereafter you can toy with interactive graphs for the principal > lightclock features: > time dilation > https://www.desmos.com/calculator/zlplep7g5k?lang=nl > length contraction > https://www.desmos.com/calculator/hpxundkvzt?lang=nl > relative simultaneity > https://www.desmos.com/calculator/7h1h4jvzno?lang=nl > > Also interesting, a difference between the mentioned "Lorentz" > properties of relativistic motion, and the properties actually "seen > when looking at" such motion. Other files about this theme, in my desmos > space. > > -- > guido wugi "Suffer" is the word! Thanks for the data, but there is no need to suffer any transformation because ordinary additive velocity is exactly correct for light, whether it is particles or waves or a hybrid. Relativity unnecessarily complicates simple matters.
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| From | Richard Hachel <r.hachel@frite.fr> |
|---|---|
| Date | 2023-07-11 18:17 +0000 |
| Message-ID | <fViD08BMqJwIa0ptNbrpTyZUY9E@jntp> |
| In reply to | #615008 |
Le 11/07/2023 à 19:56, Laurence Clark Crossen a écrit : > On Monday, July 10, 2023 at 12:52:57 PM UTC-7, wugi wrote: >> Op 9/07/2023 om 19:56 schreef Laurence Clark Crossen: >> > Design of a light clock that works on a spaceship traveling at near the speed >> of light: >> > Orient a light clock horizontally like the beam in the MMX directed in the >> direction of Earth's orbital motion. >> > The beam going out to the mirror is in the direction of the spaceship's >> motion. >> > That beam covers a longer distance since that mirror is moving away >> > On the return trip, it covers a shorter distance because the other side of the >> clock is moving towards it. >> > Result: The clock functions at the same rate as when stationary. >> > Further: This works whether light shares the velocity of the source or not. >> > Question: Why did Einstein choose a clock that doesn't work when an available >> one does? >> Light clocks deserve indeed to be considered as *the* measuring and >> calibrating tools for both time and space in SRT. They allow even an >> axiomatic approach that is intuitive, and yields constant light speed as >> a provable result, rather than it being a counterintuitive axiom, as in >> the original formulation. But then it takes understanding their functioning. >> >> "Your" light clock works only for particle behaviour of light, with >> added velocities. Then you get indeed this: >> https://wugi.be/giffls/tik19.htm >> and tN = t'N'. >> But with wave/particle behaviour this is no longer true. Looking at such >> light clocks we see, >> first, that a "moving" light clock must suffer time dilation (longer >> light path perpendicular to direction of motion); >> then, that they must suffer length contraction (for parallel en >> perpendicular light paths to "ticktock" in pace: one wants *time* to be >> an isotropic feature); >> As a result we get this correct spacetime diagram for light clocks: >> https://wugi.be/giffls/tik22.htm. >> >> Furthermore, we see, >> that simultaneity is different in a "moving" system; >> and again, that these features are reciprocal: "moving" and "rest" >> systems can be swapped, with reciprocal results; >> lastly, that light speed is constant: light clocks measure by definition >> light speed as the ratio of corresponding ticktock lengths and time >> intervals! >> One can even deduce relativistic mass from light clock behaviour, by >> considering corresponding wavelengths and the light impulses involved. >> >> Hereafter you can toy with interactive graphs for the principal >> lightclock features: >> time dilation >> https://www.desmos.com/calculator/zlplep7g5k?lang=nl >> length contraction >> https://www.desmos.com/calculator/hpxundkvzt?lang=nl >> relative simultaneity >> https://www.desmos.com/calculator/7h1h4jvzno?lang=nl >> >> Also interesting, a difference between the mentioned "Lorentz" >> properties of relativistic motion, and the properties actually "seen >> when looking at" such motion. Other files about this theme, in my desmos >> space. >> >> -- >> guido wugi > "Suffer" is the word! Thanks for the data, but there is no need to suffer any > transformation because ordinary additive velocity is exactly correct for light, > whether it is particles or waves or a hybrid. Relativity unnecessarily complicates > simple matters. It's the opposite. It's the simple things that complicate things, because they're wrong. Some want, today, to make things very simple and very practical, by adding speeds of the type v(+)u=v+u. But that is not true. Ginette Feuillebois also wants to make things very simple and very practical in her college courses. She teaches that it is more practical to simply add the two sides of the right triangle to obtain the hypothenuse. It therefore sets h=a+b and no longer h=sqrt(a²+b²) It's simpler and more convenient. But that is not true. I have given the formula for the general addition of observable relativized velocities. <http://news2.nemoweb.net/jntp?fViD08BMqJwIa0ptNbrpTyZUY9E@jntp/Data.Media:1> I even gave the equation for the addition of real speeds (it's even more complicated). <http://news2.nemoweb.net/jntp?fViD08BMqJwIa0ptNbrpTyZUY9E@jntp/Data.Media:2> Well, there will always be people who will say no. Some saying that I'm wrong (because they're uneducated cranks) and that simply w=v+u. The others more posh, because professor of faculty, saying that I am also wrong, because even if my equations are correct and universal, I have no right to speak about it. That's how it works. R.H.
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| From | Tom Roberts <tjoberts137@sbcglobal.net> |
|---|---|
| Date | 2023-07-11 13:22 -0500 |
| Message-ID | <w4WcnR_mmt9NADD5nZ2dnZfqlJ_-fwAA@giganews.com> |
| In reply to | #615008 |
On 7/11/23 12:56 PM, Laurence Clark Crossen wrote: > [...] there is no need to suffer any transformation because ordinary additive velocity is exactly correct for light, whether it is particles or waves or a hybrid. Relativity unnecessarily complicates simple matters. In the fantasy world of your own mind, that may well be true (nobody else can know, of course). In the world we inhabit, this is blatantly false. Tom Roberts
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| From | Maciej Wozniak <maluwozniak@gmail.com> |
|---|---|
| Date | 2023-07-11 13:02 -0700 |
| Message-ID | <404fd549-e697-4708-8f6e-8117ce6a1d8cn@googlegroups.com> |
| In reply to | #615012 |
On Tuesday, 11 July 2023 at 20:22:20 UTC+2, Tom Roberts wrote: > On 7/11/23 12:56 PM, Laurence Clark Crossen wrote: > > [...] there is no need to suffer any transformation because ordinary additive > velocity is exactly correct for light, whether it is particles or waves > or a hybrid. Relativity unnecessarily complicates simple matters. > In the fantasy world of your own mind, that may well be true (nobody > else can know, of course). In the world we inhabit we're FORCED!!! to THE BEST WAY!!!
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